Transmission type spatial light modulator and transmission type spatial light modulation array device
Summary by NHIP
Oblique Displacement Spatial Light Modulator
The apparatus deflects incident light using a minute transparent optical member supported in a midair position. A driving member obliquely displaces this member via electrical mechanical operation to vary the light emission direction relative to a perpendicular plane.
Claim Score by NHIP
Abstract
A transmission type spatial light modulatoris equipped with a minute transparent optical member for deflecting light in a direction different from an incident direction of incident light and emitting the light, a support member for supporting the minute transparent optical member at a midair position so that the light emission face can be inclined with respect to a plane perpendicular to a travel direction of incident light L1, and a driving member for obliquely displacing the minute transparent optical member by an electrical mechanical operation to vary the emission direction of light from the minute transparent optical member.

Term
Term ended
Expired 28 February 2026, 0.6 years ago.
- Priority
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30 claims: 1 independent, 29 dependent
- 1Broadest claimClaim Score 69, broad(NHIP)A transmission type spatial light modulator comprising:an optical member that deflects and emits light in a direction different from an incident direction of incident light;a support member that supports the optical member in a midair position so that a light emission face thereof can be inclined with respect to a plane perpendicular to a travel direction of the light incident direction;and driving member that obliquely displaces the optical member to vary the light emission direction from the optical member.
197 paragraphs in 4 sections, as filed
This application is based on Japanese Patent application JP 2004-168097, filed Jun. 7, 2004, the entire content of which is hereby incorporated by reference. This claim for priority benefit is being filed concurrently with the filing of this application.
BACKGROUND OF THE INVENTION
1. Technical Field of the Invention
The present invention relates to a transmission type spatial light modulator and a transmission type spatial light modulation array device.
2. Description of the Related Art
A light deflector is known as a device for controlling any one of an angle or position of a light propagation direction or both the angle and the position with respect to the time. As the light deflector are known a reflection type mechanical type light deflector for deflecting light by swinging a reflection mirror, and a transmission type mechanical type light deflector for deflecting light by rotating a prism or the like. In the reflection type, incident light and emission light exist at the same side with respect to the device. On the other hand, in the transmission type, the incident light and the emission light exist at the different sides with respect to the device, and thus it has an advantage that the construction of the peripheral optical system is simple. For example, in the construction disclosed in JP-A-11-249037, PBS (Polarized beam splitter) is disposed to make light from a light source incident to a reflection type spatial light modulation array device. However, it is not needed in the transmission type. In the construction disclosed in JP-A-2001-201716, surface reflection light from a reflection type spatial light modulation array device (micro-mirror device) is unnecessary light, and it reduces the contrast, so that a light separating prism provided to prevention the reduction of the contrast enlarges the device.
In the reflection type, since the incident light and the emission light (deflected light) and the unnecessary light such as the surface reflection light based on the incident light exist at the same side with respect to the device, it is difficult to freely set the directions of ON light (effective light) and OFF light (unnecessary light) in the emission light (deflected light). For example, when great importance is placed on the contrast, it is required that the directions of the ON light and the unnecessary light such as the surface reflection light, etc. are different from each other. On the other hand, in the transmission type, the unnecessary light such as the surface reflection light, etc. based on the incident light exists at the incident side, and only the emission light (deflected light) exists at the emission side, so that it is possible to freely set the directions of the ON light and the OFF light in the emission light. Therefore, the degree of freedom of the design of a peripheral optical system is enhanced, and the latitude of the optical precision is relatively enhanced. An example of a conventional transmission type mechanical light deflector will be described. In this specification, “deflection” means the function of controlling any one of the angle and position of the light propagation direction or both the angle and the position with respect to the time.
An optical switch disclosed in JP-A-2002-23072 is equipped with a plurality of light input/output portions <b>1</b> comprising optical fibers for transmitting optical signals, deflecting means (wedged prism) <b>3</b> for deflecting a light beam corresponding to an optical signal incident from the light input/output portion <b>1</b> and selecting an optical fiber of the light input/output portion <b>1</b> to which the optical signal should be transmitted, and light converging means <b>5</b><i>a</i>, <b>5</b><i>b </i>for converging the light beam corresponding to the optical signal incident/emitted to/from the optical input/output portion <b>1</b> to set the optical beam to a collimated beam, and converging the light beam emitted from the deflecting means <b>3</b> into the optical fiber of the light input/output portion <b>1</b> selected by the deflecting means <b>3</b> as shown in <figref idref="DRAWINGS">FIG. 36</figref>.
According to the optical switch, since a light beam is deflected and an optical fiber to which the light should be made incident is selected by rotating the wedge-shaped prism <b>3</b>, there can be achieved effects that the optical fiber itself is not required to be moved, and thus the optical fiber can be prevented from being damaged by the movement of the optical fiber, so that the reliability of light transmission can be enhanced.
As shown in <figref idref="DRAWINGS">FIGS. 37A to 37B</figref>, a beam deflecting device disclosed in JP-A-2000-180742 is equipped with a rotating prism body <b>7</b> that is formed of an optical material and has two or more pairs of a light incident face and a light emission face which are arranged in parallel so as to face each other, and a rotationally driving device for rotating the light incident faces <b>7</b><i>a </i>to <b>7</b><i>c </i>and the light emission faces <b>7</b><i>d </i>to <b>7</b><i>f </i>around the rotational axial line, and by rotating the rotational prism body <b>7</b> around the rotational axial line R, a light beam which is incident along the optical axis O directing to the rotational axial line to the light incident faces <b>7</b><i>a </i>to <b>7</b><i>c </i>within a plane which is vertical to the light incident faces <b>7</b><i>a </i>to <b>7</b><i>c</i>, the light emission faces <b>7</b><i>d </i>to <b>7</b><i>f </i>and the rotational axial line R is emitted from the confronting light emission faces <b>7</b><i>d </i>to <b>7</b><i>f </i>as a light beam parallel to the optical axis O, the distance of the light beam from the optical axis varying with respect to the time.
According to the beam deflecting device, the rotational prism body <b>7</b> having two or more pairs of optical faces which are arranged in parallel so as to face each other is used, and a light beam parallel to the optical axis O, the distance thereof from the optical axis varying with respect to the time is emitted, so that a long scan width can be achieved without increasing the weight of the rotational prism body <b>7</b>.
In an apex-angle variable prism device disclosed in JP-A-8-5942, the peripheries of two confronting glass plates <b>9</b>, <b>11</b> are covered by a bellows <b>13</b>, and transparent liquid <b>14</b> such as silicon oil or the like is closely sealed therein. The two confronting glass plates <b>9</b>, <b>11</b> are relatively inclined and the apex angle between the two glass plates <b>9</b>, <b>11</b> is made variable as shown in <figref idref="DRAWINGS">FIGS. 38A and 38B</figref>. In <figref idref="DRAWINGS">FIG. 38A</figref>, the two glass plates <b>9</b> and <b>11</b> are kept in parallel, and in this case, the incident angle and the emission angle of a light beam <b>15</b> to/from the apex-angle variable prism are equal to each other. On the other hand, when they intersects to each other at an angle as shown in <figref idref="DRAWINGS">FIG. 38B</figref>, the light beam is bent at some degree as indicated by the light beam <b>15</b>.
According to the apex-angle variable prism device, when a camera is inclined due to shaking or the like, the angle (apex angle) of the apex-angle variable prism provided in front of a photographing lens is controlled so that the light beam <b>15</b> corresponding to the inclination angle is bent, thereby removing blurring.
As shown in <figref idref="DRAWINGS">FIG. 39</figref>, a light deflecting device disclosed in JP-A-11-149050 has a semi-spherical body <b>17</b> comprising a plane portion for refracting/deflecting an incident light beam and a semi-spherical portion facing the plane portion so that the plane portion is wrapped by the semi-spherical portion, a support member <b>19</b> for supporting the semi-spherical body <b>17</b> so that the semi-spherical body <b>17</b> is freely rotatable and driving members <b>21</b>, <b>23</b> for rotating the semi-spherical body <b>17</b>. The semi-spherical body <b>17</b> has a solid body, and is formed of a material through which a light beam to be deflected is transmissible. In addition, the plane portion and a space or medium <b>25</b> which comes into contact with the plane portion are different in refractive index.
According to this light deflecting device, the light deflection is carried out mechanically, and thus it is possible to set a large deflection angle θ in a three-dimensional free direction. Furthermore, arrangements at the incident side and emission side can be achieved along the transmission direction, and thus the whole device can be miniaturized.
However, the optical switch disclosed in JP-A-2002-23072, the beam deflecting device disclosed in JP-A-2000-180742 and the apex-angle variable prism device disclosed in JP-A-8-5942 are unsuitable structurally or as a driving-mechanism for the construction of the minute transmission type spatial light modulator for carrying out light deflection on a pixel basis in an exposure head, a display or the like, and it is difficult to carry out a low-voltage driving operation by any disclosed driving members even if miniaturization thereof is possible. On the other hand, the light deflecting device disclosed in JP-A-11-149050 is applicable as a minute transmission type spatial light modulator. However, since the support portion thereof is filled with lubricant, it is estimated that the response is lowered by the friction thereof. Furthermore, it has low resistance to shock and temperature variation, and thus there is a risk that it has low reliability and a short lifetime. Under such a condition, it is necessarily and unavoidably difficult to apply this light deflecting device to an exposure head, a display or the like which needs high-speed response deflection of μs-order and a semi-permanent operation. Furthermore, an extremely high precision manufacturing technique is required to form a high-precision semi-spherical structure which is directly associated with the stable performance of the rotational operation of the semi-spherical body and the recess structure of the surrounding portion which is matched with the structure of the semi-spherical body. Therefore, when it is applied to an exposure head, a display or the like, it is estimated that it is realistically difficult in yield to manufacture a transmission type spatial light modulation array device in which transmission type spatial light modulators each having a large number of pixels are arranged. The present invention has been implemented in view of the foregoing situation.
SUMMARY OF THE INVENTION
An object of the invention is to provide a transmission type spatial light modulator and a transmission type spatial light modulation array device that can perform high-speed deflection and a low-voltage driving operation, further miniaturize elements and enhance the contrast by suppressing stray light or unnecessary light. The object can be attained by adoption of the following constitution.
(1). A transmission type spatial light modulator comprising: a minute transparent optical member for deflecting and emitting light in a direction different from the incident direction of incident light; a support member for supporting the minute transparent optical member in a midair position so that a light emission face thereof can be inclined with respect to a plane perpendicular to a travel direction of the light incident direction; and a driving member for obliquely displacing the minute transparent optical member by an electrical mechanical operation to vary the light emission direction from the minute transparent optical member.
In the transmission type modulator, the direction and light amount of transmission light can be controlled by a small displacement amount. Furthermore, emission light is directed in the same travel direction as incident light, and an optical system which is needed in the case of a reflection type modulator is not required. In addition, the separation between ON light and OFF light can be more easily performed as compared with the reflection type modulator. Furthermore, the wavelength-dependence is lowered as compared with an interference type spatial light modulator using the Fabry-Perot effect or the like.
(2). The transmission type spatial light modulator according to (1), further comprising a light shielding member that is disposed ahead of the light emission face of the minute transparent optical member and shields any emission light in a direction-variable range of light emitted from the minute transparent optical member.
In the transmission type spatial light modulator, a desired area in the direction variable range of light emitted from the minute transparent optical member can be set to a light transmission area or a light shielding area.
(3). The transmission type spatial light modulator according to (2), wherein the driving member obliquely displaces the minute transparent optical member to displace the emission light with respect to the light shielding member, thereby varying the transmission light amount of the emission light.
In this transmission type spatial light modulator, ON/OFF of light intensity and a switching operation of a route can be performed in cooperation with a light deflecting operation based on the oblique displacement of the minute transparent optical member.
(4). The transmission type spatial light modulator according to anyone of (1) to (3), wherein the minute transparent optical member has a refractive index larger than 1 and light incident and emission faces are formed by non-parallel faces.
In this transmission type spatial light modulator, the minute transparent optical member can be formed of a structure having a single refractive index. The emission angle of the deflected light can be freely set by merely controlling the design of the inclination angles of the light incident and emission faces.
(5). The transmission type spatial light modulator according to any one of (1) to (4), wherein the minute transparent optical member has a refractive index distribution different in refractive index in accordance with the light travel direction, and a light deflection direction based on the refractive index distribution is different from the light travel direction.
In this transmission type spatial light modulator, the deflection range can be arbitrarily set by using a flat-plate type minute transparent optical member. Furthermore, the thickness of the minute transparent optical member can be reduced.
(6). The transmission type spatial light modulator according to any one of (1) to (4), wherein the minute transparent optical member has a total reflection face for totally reflecting the incident light.
In this transmission type spatial light modulator, the total reflection of the incident light is possible in addition to the deflection of the incident light. Accordingly, the deflected light is emitted from the opposite side to the light incident face of the minute transparent optical member, and the reflected light is emitted from the light incident face side of the minute transparent optical member, so that the effective light (ON light) and the unnecessary light (OFF light) are separated to the opposite sides with respect to the minute transparent optical member.
(7). The transmission type spatial light modulator according to (6), wherein the minute transparent optical member is obliquely displaced by the driving member to transmit or totally reflect the incident light.
In this transmission type spatial light modulator, the minute transparent optical member is obliquely displaced so that the incident angle of the incident light incident to the total reflection surface is smaller or larger than the critical angle, whereby the ON light and the OFF light are separated to the opposite sides with respect to the minute transparent optical member. Furthermore, since the total reflection is carried out by the total reflection surface formed in the minute transparent optical member, so that internal total reflection (Total Internal Reflection) can be performed and thus light absorption can be reduced as compared with the reflection on the total reflection surface.
(8). The transmission type spatial light modulator according to (7), further comprising an optical path correcting member that is disposed ahead of the light emission face of the minute transparent optical member to make an incident angle and an emission angle substantially coincident with each other.
In this transmission type spatial light modulator, the emission light (ON light) which is separated to the opposite side to the incident light with respect to the minute transparent optical member can straightly travel in the same direction as the incident light.
(9). The transmission type spatial light modulator according to any one of (6) to (8), wherein the minute transparent optical member is designed in a prism-shape.
In this transmission type spatial light modulator, a large deflection angle can be achieved by a small inclination angle. Furthermore, the reflection loss can be reduced, and the light absorption can be reduced as compared with the reflection on the metal surface. Still furthermore, since the deflection angle is large, it is easy to take a margin, and the degree of freedom of an optical design of an optical path or the like can be enhanced.
(10). The transmission type spatial light modulator according to (6) to (8), wherein at least a part of the light incident face or light emission face of the minute transparent optical member is designed in a curved-surface shape.
In this transmission type spatial light modulator, the refractive index is continuously varied, and the refractive index difference in the refractive index variation range is set to a large value.
(11). The transmission type spatial light modulator according to (1), further comprising: a first prism member for receiving the emission light when the minute transparent optical member is obliquely displaced by the driving member and the emission light is emitted from the minute transparent optical member in a predetermined direction, and emitting the emission light as effective light while deflecting the emission light in a first direction; and a second prism member for receiving the emission light when the minute transparent optical member is obliquely displaced by the driving member and the emission light is emitted from the minute transparent optical member in a direction different from the predetermined direction, and deflecting the emission light as unnecessary light in a second direction different from the first direction.
In this transmission type spatial light modulator, the emission directions of the effective light and the unnecessary light can be made greatly different by the first prism member and the second prism member, and for example, they can be made to the opposite directions.
(12). The transmission type spatial light modulator according to any one of (1) to (11), wherein the driving member obliquely displaces the minute transparent optical member by electrostatic force.
In this transmission type spatial light modulator, the minute transparent optical member can be electrically and mechanically operated at a high speed and with a low voltage to be obliquely displaced by electrostatic suction force caused by electrostatically-induced charges.
(13). A transmission type spatial light modulation array device comprising transmission type spatial light modulators according to anyone of (1) to (12), the transmission type spatial light modulators being arranged one-dimensionally or two-dimensionally.
In this transmission type spatial light modulation array device, the transmission type spatial light modulators having the same structure are arranged one-dimensionally or two-dimensionally, and function as one light modulation device. Therefore, high-density pixels can be subjected to light modulation at high speed in an application to an exposure head, a display or the like. Furthermore, the many transmission type spatial light modulators can be arranged with the same quality and high precision by a semiconductor manufacturing process.
(14). The transmission type spatial light modulation array device according to (13), wherein a micro-lens array having a plurality of micro-lenses disposed in connection with the respective transmission type spatial light modulators is disposed so as to confront the light incident face.
In this transmission type optical array device, incident light flux is converged, so that the minute transparent optical member can be miniaturized and reduced in weight. Furthermore, as compared with a case where no micro-lens is used, a minute transparent optical member having a small area can be formed, and thus a driving circuit area can be secured in the comparison of the same substrate area.
According to the transmission type spatial light modulator of the present invention, the minute transparent optical member for emitting light therefrom in a direction different from incident light is supported by the support member so as to be inclined, and the minute transparent optical member is obliquely displaced by the electrical mechanical operation of the driving member to vary the light emission direction. Therefore, the direction of the transmitted light and the light amount of the transmitted light can be controlled by a small displacement amount, and the high-speed deflection and the low-voltage driving operation can be implemented. Accordingly, a low power consumption driving operation can be performed. Furthermore, in the case of the reflection type spatial light modulator, the light incident path and the light reflection path to the modulator exist at the same surface side, and thus an optical system for avoiding the interference between both the optical paths is needed. However, according to the transmission type spatial light modulator of the present invention, the light emission light is directed in the travel direction of the incident light, so that the optical system needed in the case of the reflection type modulator is unnecessary. Accordingly, in the transmission type spatial light modulator of this invention, the construction of the peripheral optical system can be simplified, and thus the spatial light modulator can be miniaturized. Furthermore, the separation between the ON light and the OFF light can be more easily performed as compared with the reflection type spatial light modulator, and thus stray light and unnecessary light can be suppressed a and the contrast can be enhanced. Still furthermore, the wavelength-dependence which is observed in an interference type spatial light modulator using Fabry-Perot effect or the like can be eliminated.
According to the transmission type spatial light modulation array device of the present invention, the transmission type spatial light modulators are one-dimensionally or two-dimensionally arranged. Therefore, the transmission type spatial light modulators having the same structure are one-dimensionally or two-dimensionally arranged on the same substrate, and thus they function as one light modulation device, so that high-density pixels can be subjected to light modulation at high speed in an application to an exposure head, a display or the like. Furthermore, many transmission type spatial light modulators can be arranged with the same quality and with high precision by the semiconductor manufacturing process, so that the light emission light can be aligned and image display, etc. can be performed with high quality and high resolution.
BRIEF DESCRIPTION OF THE DRAWINGS
<figref idref="DRAWINGS">FIG. 1</figref> is a perspective view showing a first embodiment of a transmission type spatial light modulator according to the present invention.
<figref idref="DRAWINGS">FIGS. 2A and 2B</figref> are cross-sectional views showing (<figref idref="DRAWINGS">FIG. 2A</figref>) an initial state and (<figref idref="DRAWINGS">FIG. 2B</figref>) an operation state of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIGS. 3A to 3C</figref> are diagrams showing the relationship between the inclination angle and the emission angle of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIGS. 4A to 4D</figref> are diagrams showing the principle of emission angle control based on the oblique displacement of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIG. 5</figref> is an enlarged view showing a main part of a minute transparent optical member shown in <figref idref="DRAWINGS">FIGS. 4A to 4D</figref>.
<figref idref="DRAWINGS">FIG. 6</figref> is a diagram showing the correlation between the emission angle and the rotational angle in the transmission type spatial light modulator (in the case of refractive index n=1.5) shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIG. 7</figref> is an enlarged view showing a main range of <figref idref="DRAWINGS">FIG. 6</figref>.
<figref idref="DRAWINGS">FIG. 8</figref> is a diagram showing the correlation between the emission angle and the rotational angle in the transmission type spatial light modulator (in the case of the refractive index n=2.03)shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIG. 9</figref> is an enlarged view showing a main range of <figref idref="DRAWINGS">FIG. 8</figref>.
<figref idref="DRAWINGS">FIG. 10</figref> is a plan view showing transmission type spatial light modulators shown in <figref idref="DRAWINGS">FIG. 1</figref> which correspond to four pixels.
<figref idref="DRAWINGS">FIG. 11</figref> is a cross-sectional view taken along XI-XI line of <figref idref="DRAWINGS">FIG. 10</figref>.
<figref idref="DRAWINGS">FIG. 12</figref> is a cross-sectional view taken along XII-XII line of <figref idref="DRAWINGS">FIG. 10</figref>.
<figref idref="DRAWINGS">FIGS. 13A and 13B</figref> are diagrams showing the operation of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>.
<figref idref="DRAWINGS">FIGS. 14A to 14H</figref> are diagrams showing the manufacturing process of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref> in the same cross-sectional view as <figref idref="DRAWINGS">FIG. 11</figref>.
<figref idref="DRAWINGS">FIGS. 15A to 15H</figref> are diagrams showing the manufacturing process of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref> in the same cross-sectional view as <figref idref="DRAWINGS">FIG. 12</figref>.
<figref idref="DRAWINGS">FIG. 16</figref> is an electrode wire diagram showing a second embodiment of the transmission type spatial light modulator of the present invention.
<figref idref="DRAWINGS">FIG. 17</figref> is a diagram showing the operation representing a left-side inclination condition of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 16</figref>.
<figref idref="DRAWINGS">FIG. 18</figref> is a diagram showing the operation representing a right-side inclination condition of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 16</figref>.
<figref idref="DRAWINGS">FIGS. 19A and 19B</figref> are cross-sectional views representing a modification <b>1</b> of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 16</figref> in which a minute transparent optical member is displaced by a flexible flat plate.
<figref idref="DRAWINGS">FIG. 20</figref> is a perspective view showing a modification <b>2</b> of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 16</figref> which is equipped with a comb-drive.
<figref idref="DRAWINGS">FIGS. 21A to 21C</figref> are cross-sectional views showing a third embodiment having a light shielding member.
<figref idref="DRAWINGS">FIGS. 22A and 22B</figref> are cross-sectional views showing a modification of the third embodiment in which the position of the light shielding member is different.
<figref idref="DRAWINGS">FIGS. 23A and 23B</figref> are cross-sectional views showing a fourth embodiment in which the minute transparent optical member has a total reflection face.
<figref idref="DRAWINGS">FIGS. 24A and 24B</figref> are cross-sectional views showing a modification of the fourth embodiment in which the shape of the minute optical member is different.
<figref idref="DRAWINGS">FIGS. 25A to 25D</figref> are cross-sectional views showing a fifth embodiment using a prism as the minute transparent optical member.
<figref idref="DRAWINGS">FIG. 26</figref> is a cross-sectional view showing a modification <b>1</b> of the fifth embodiment which has an optical path correcting member.
<figref idref="DRAWINGS">FIG. 27</figref> is a cross-sectional view showing a modification <b>2</b> of the fifth embodiment which uses a parallelogram prism.
<figref idref="DRAWINGS">FIGS. 28A to 28C</figref> are cross-sectional views showing a sixth embodiment in which the light emission face of the minute transparent optical member is designed in a curved-surface shape.
<figref idref="DRAWINGS">FIGS. 29A to 29C</figref> are cross-sectional views showing a seventh embodiment in which the minute transparent optical member has a refractive index distribution.
<figref idref="DRAWINGS">FIGS. 30A to 30C</figref> are cross-sectional views showing a modification of the seventh embodiment in which the refractive interface is designed in a curved-surface shape.
<figref idref="DRAWINGS">FIG. 31</figref> is a cross-sectional view of the transmission type spatial light modulation array device according to an eighth embodiment which aims at integration of micro-lenses.
<figref idref="DRAWINGS">FIG. 32</figref> is a cross-sectional view showing a modification of the transmission type spatial light modulation array device shown in <figref idref="DRAWINGS">FIG. 31</figref> which is equipped with two-stage micro-lenses.
<figref idref="DRAWINGS">FIG. 33</figref> is a diagram showing the construction of an exposure device according to a ninth embodiment using the transmission type spatial light modulation array device.
<figref idref="DRAWINGS">FIG. 34</figref> is a block diagram showing the exposure device shown in <figref idref="DRAWINGS">FIG. 33</figref>.
<figref idref="DRAWINGS">FIG. 35</figref> is a diagram showing the optical path of the exposure device shown in <figref idref="DRAWINGS">FIG. 33</figref>.
<figref idref="DRAWINGS">FIG. 36</figref> is a schematic diagram showing an optical switch serving as a conventional transmission type mechanical light deflector.
<figref idref="DRAWINGS">FIG. 37</figref> is a diagram showing the construction of a main part of a beam deflecting device serving as a conventional transmission type mechanical light deflector.
<figref idref="DRAWINGS">FIG. 38</figref> is a diagram showing the construction of a main part of an apex-angle variable prism device serving as a conventional transmission type mechanical light deflector.
<figref idref="DRAWINGS">FIG. 39</figref> is a diagram showing the construction of a main part of a light deflecting device serving as a conventional transmission type mechanical light deflector.
Reference numerals are used to identify various elements in the drawings including the following: <ul id="ul0001" list-style="none"><li id="ul0001-0001" num="0087"><b>32</b> hinge (support member)</li><li id="ul0001-0002" num="0088"><b>33</b>, <b>85</b>, <b>99</b>, <b>103</b> minute transparent optical member</li><li id="ul0001-0003" num="0089"><b>35</b> driving member</li><li id="ul0001-0004" num="0090"><b>71</b> flexible flat plate (support member)</li><li id="ul0001-0005" num="0091"><b>77</b> swing shaft (support member)</li><li id="ul0001-0006" num="0092"><b>83</b> light shielding member</li><li id="ul0001-0007" num="0093"><b>89</b> emission face (total reflection face)</li><li id="ul0001-0008" num="0094"><b>91</b>, <b>141</b> optical path correcting member</li><li id="ul0001-0009" num="0095"><b>100</b>, <b>180</b>, <b>200</b>, <b>300</b>, <b>400</b>, <b>500</b>, <b>600</b> transmission type spatial light modulator</li><li id="ul0001-0010" num="0096"><b>117</b> micro-lens array</li><li id="ul0001-0011" num="0097"><b>117</b><i>a </i>micro-lens</li><li id="ul0001-0012" num="0098"><b>700</b>, <b>900</b> transmission type spatial light modulation array device</li><li id="ul0001-0013" num="0099">L<b>1</b> incident light</li><li id="ul0001-0014" num="0100">L<b>2</b> emission light</li></ul>
DETAILED DESCRIPTION OF THE INVENTION
Preferable embodiments of a transmission type spatial light modulator and a transmission type spatial light modulation array device according to the present invention will be described in detail with reference to the drawings.
<figref idref="DRAWINGS">FIG. 1</figref> is a perspective view showing a first embodiment of the transmission type spatial light modulator according to the present invention, and <figref idref="DRAWINGS">FIGS. 2A to 2B</figref> are cross-sectional showing an initial state (<figref idref="DRAWINGS">FIG. 2A</figref>) and an operation state (<figref idref="DRAWINGS">FIG. 2B</figref>) of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>.
A transmission type spatial light modulator <b>100</b> according to an embodiment has a substrate <b>31</b>, a minute transparent optical member <b>33</b> mounted on the substrate <b>31</b>, a hinge (support member) <b>32</b> for supporting the minute transparent optical member <b>33</b> at both the side portions thereof, and a driving member <b>35</b> for obliquely displacing the minute transparent optical member <b>33</b> as basic constituent elements as shown in <figref idref="DRAWINGS">FIG. 1</figref> and <figref idref="DRAWINGS">FIGS. 2A and 2B</figref>.
The minute transparent optical member <b>33</b> works to deflect light in a direction different from an incident direction of incident light L<b>1</b>. The minute transparent optical member <b>33</b> comprises movable film <b>37</b> having an electrically conductive portion described later formed at at least a part thereof, and a deflecting portion <b>39</b> provided on the upper surface of the thin film portion <b>37</b>. The deflecting portion <b>39</b> may be a minute prism formed of glass, for example. The movable film <b>37</b> and the deflecting portion <b>39</b> may be formed separately from each other or integrally with each other.
The hinge <b>32</b> supports the minute transparent optical member <b>33</b> so that the movable film <b>37</b> is spaced from the substrate <b>31</b> through a gap <b>51</b> in parallel to the substrate <b>31</b> as shown in <figref idref="DRAWINGS">FIG. 2A</figref>, and also supports the minute transparent optical member <b>33</b> at a midair position so that the light emission face (the upper surface of the deflecting portion <b>39</b>) is further inclined with respect to a plane perpendicular to the travel direction of incident light (that is, the surface of the substrate <b>31</b>) as shown in <figref idref="DRAWINGS">FIG. 2B</figref> when force is applied in a distortion direction by a driving member <b>35</b>.
The transmission type spatial light modulator <b>100</b> is designed, for example, so that the pixel area is set to 20 μm×20 μm in size, the movable film <b>37</b> is set to 10 μm×5 μm in size and the height of the short side of the deflecting portion <b>39</b> is set to about 3 to 4 μn.
The driving member <b>35</b> obliquely displaces the minute transparent optical member <b>33</b> by an electrical mechanical operation to greatly vary the emission direction of light from the minute transparent optical member <b>33</b> as shown in <figref idref="DRAWINGS">FIG. 2B</figref>. The driving member <b>35</b> has an electrically conductive portion provided to the movable film <b>37</b> (a voltage Vm is applied to the electrically conductive portion, and even in the construction that the electrically conductive portion is added to the movable film <b>37</b>, the movable film <b>37</b> itself may be formed of electrically conductive film), and lower electrodes <b>53</b>, <b>54</b> which are disposed at the substrate <b>31</b> side and confront the movable film <b>37</b> through the above gap <b>51</b>. The lower electrodes <b>53</b>, <b>54</b> are arranged at both the sides between which the hinge <b>32</b> is sandwiched, and voltages V<b>1</b> and V<b>2</b> are applied to the lower electrodes <b>53</b>, <b>54</b>, respectively.
Any material such as a glass substrate or the like may be used as the substrate <b>31</b> in so far as it is transparent to incident light. Even when it is an opaque substrate such as a Si substrate or the like, it is usable by providing a light transmissible property to only an area where incident light is deflected. Specifically, it is preferable that circuits (normally, a CMOS circuit and a wiring circuit therefor) for driving a device is formed on the Si substrate, the upper surface thereof is flattened by an insulating layer and an opening hole is formed at the area where the light deflection is carried out. The movable film <b>37</b> and the lower electrodes <b>53</b>, <b>54</b> are provided on the upper surface of the flattened insulating layer, and these are electrically connected to one another through contact holes (not shown) provided in the insulating layer. These structures will be described in detail later.
<figref idref="DRAWINGS">FIGS. 3A to 3B</figref> are diagrams showing the relationship between the inclination angle and the emission angle of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>. In the transmission type spatial light modulator <b>100</b>, for example when the prism angle (the intersecting angle between the incident face and the emission face) θo of a triangular deflecting portion <b>39</b> having a refractive index n=1.5 is equal to 30°, the inclination angle θr=0° and the emission angle θe of the deflected light is slightly less than 20° under an initial state where the driving member <b>35</b> is not actuated as shown in <figref idref="DRAWINGS">FIG. 3B</figref>. Furthermore, as shown in <figref idref="DRAWINGS">FIG. 3A</figref>, when the driving member <b>35</b> is actuated and the inclination angle θr=−15°, the incident angle of the incident light to the emission face is increased, and thus the emission angle θe of the deflected light emitted from the emission face is greatly varied to 30°. In this specification, the clockwise rotation is set as a positive-direction rotation, and the counterclockwise rotation is set as a negative-direction rotation and thus it is added with a minus sign. Furthermore, as shown in <figref idref="DRAWINGS">FIG. 3C</figref>, even when the driving member <b>35</b> is actuated and the inclination angle θr=15°, the emission angle θe of the deflected light is equal to slightly less than 15°, and the emission angle θe is not so different angle from that under the state of <figref idref="DRAWINGS">FIG. 3A</figref>. In the figures, <b>57</b> represents a transparent front-surface protection substrate disposed at the opposite side to the substrate <b>31</b> through the minute transparent optical member <b>33</b> so as to confront the substrate <b>31</b>.
<figref idref="DRAWINGS">FIGS. 4A to 4D</figref> are diagrams showing the principle of emission angle control on the basis of inclination displacement of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIG. 1</figref>, and <figref idref="DRAWINGS">FIG. 5</figref> is an enlarged view showing the main part of the minute transparent optical member shown in <figref idref="DRAWINGS">FIG. 1</figref>. At least the deflecting portion <b>39</b> of the minute transparent optical member <b>33</b> has a refractive index n larger than 1, and the light incident face and the light emission face are formed of non-parallel faces. The minute transparent optical member <b>33</b> is formed of a structure having a single refractive index, whereby the spatial light modulator can be easily formed. Furthermore, the emission angle of the deflected light can be freely set by merely controlling the design of the inclination angle (prism angle) of the light incident face and the light emission face, and the spatial light modulator having a desired deflection angle can be easily manufactured.
When the minute transparent optical member <b>33</b> is rotated in the positive direction (clockwise direction) from the initial state that the inclination angle θr shown in <figref idref="DRAWINGS">FIG. 4B</figref> is equal to zero, the transmission type spatial light modulator <b>100</b> is set to a state shown in <figref idref="DRAWINGS">FIG. 4A</figref>, and incident light is incident to the emission face substantially vertically, so that the deflection angle difference is small. On the other hand, when it is rotated in the negative direction (counterclockwise direction), the transmission type spatial light modulator <b>100</b> is set to a state shown in <figref idref="DRAWINGS">FIG. 4C</figref>, the emission angle of the deflected light is greatly varied, and when the inclination angle θr is larger than the critical angle θcc, the transmission type spatial light modulator <b>100</b> is set to a state shown in <figref idref="DRAWINGS">FIG. 4D</figref>, so that the incident light L<b>1</b> is totally reflected by the emission face, and thus is not emitted from the emission face.
The emission angle θe of the deflected light can be controlled by using the prism angle θo, the inclination angle θr and the refractive index n as parameters. That is, these values and the emission angle θe are associated with each other as shown in <figref idref="DRAWINGS">FIG. 5</figref>. That is,
<maths id="MATH-US-00001" num="00001"><math overflow="scroll"><mtable><mtr><mtd><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>a</mi></mrow><mo>=</mo><mrow><mi>arcsin</mi><mo></mo><mrow><mo>(</mo><mrow><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mrow><mi>r</mi><mo>/</mo><mi>n</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>b</mi></mrow><mo>=</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow><mo>-</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>a</mi></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>c</mi></mrow><mo>=</mo><mrow><mrow><mi>π</mi><mo>/</mo><mn>2</mn></mrow><mo>-</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>b</mi></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>π</mi><mo>/</mo><mn>2</mn></mrow><mo>-</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>-</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow><mo>-</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>b</mi></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>a</mi></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>d</mi></mrow><mo>=</mo><mrow><mi>arcsin</mi><mo></mo><mrow><mo>(</mo><mrow><mi>n</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr></mtable></math></maths>
Accordingly, the emission angle θe is represented as follows:
<maths id="MATH-US-00002" num="00002"><math overflow="scroll"><mtable><mtr><mtd><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>e</mi></mrow><mo>=</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>d</mi></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>b</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>c</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>d</mi></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>arcsin</mi><mo></mo><mrow><mo>(</mo><mrow><mi>n</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>c</mi></mrow><mo>)</mo></mrow></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>arcsin</mi><mo></mo><mrow><mo>(</mo><mrow><mi>n</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>a</mi></mrow></mrow><mo>)</mo></mrow></mrow><mo>)</mo></mrow></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr><mtr><mtd><mrow><mo>=</mo><mrow><mrow><mi>arcsin</mi><mo></mo><mrow><mo>[</mo><mrow><mi>n</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>sin</mi><mo></mo><mrow><mo>{</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>arcsin</mi><mo></mo><mrow><mo>(</mo><mrow><mi>sin</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mrow><mi>r</mi><mo>/</mo><mi>n</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow><mo>}</mo></mrow></mrow><mo>]</mo></mrow></mrow><mo>-</mo><mrow><mo>(</mo><mrow><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>o</mi></mrow><mo>+</mo><mrow><mi>θ</mi><mo></mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo></mo><mi>r</mi></mrow></mrow><mo>)</mo></mrow></mrow></mrow></mtd></mtr></mtable></math></maths>
<figref idref="DRAWINGS">FIG. 6</figref> is a diagram showing the correlation between the emission angle θe and the rotational angle (inclination angle) θr based on the above calculation equations every prism angle θo=10° in the case of the refractive index n=1.5, and <figref idref="DRAWINGS">FIG. 7</figref> is an enlarged view of the main part range of <figref idref="DRAWINGS">FIG. 6</figref>. <figref idref="DRAWINGS">FIG. 8</figref> is a diagram showing the correlation between the emission angle θe and the rotational angle (inclination angle) θr every prism angle θo=100 in the case of the refractive index n=2.03, and <figref idref="DRAWINGS">FIG. 9</figref> is an enlarged view of the main part range of <figref idref="DRAWINGS">FIG. 8</figref>.
In order to drive the transmission type spatial light modulator <b>100</b> at high speed, it is more advantageous to set the inclination angle θr to a value which is as small as possible. Therefore, the inclination angle θr =±15° is set to the upper limit of the driving range, and the prism angle θo is set to 30°, whereby 30° can be secured as the emission angle θo in the case of the refractive index n=1.5 (<figref idref="DRAWINGS">FIG. 6</figref>, <figref idref="DRAWINGS">FIG. 7</figref>). That is, the deflected light of the emission angle 30° is set as ON light (or OFF light), and the deflected light of the emission angle of 15° to 20° (see <figref idref="DRAWINGS">FIGS. 3B and 3C</figref>) is set to OFF light (or ON light), whereby the ON light and the OFF light can be easily discriminated from each other.
A higher advantage could be achieved by forming the transmission type spatial light modulator <b>100</b> of a material having a high refractive index. <figref idref="DRAWINGS">FIGS. 8 and 9</figref> show an example of the refractive index n=2.03, and as compared with <figref idref="DRAWINGS">FIGS. 6 and 7</figref>, it is sufficient to set the prism angle θo to 20° in order to secure the same emission angle θe =30°, so that the deflecting portion <b>39</b> ca be easily manufactured. As compared with <figref idref="DRAWINGS">FIGS. 6 and 7</figref>, when the deflecting portion <b>39</b> having the same prism angle is used, the driving range of the inclination angle can be further narrowed, and the higher speed driving can be performed. Furthermore, by securing a larger emission angle θe, the discrimination between the ON light and the OFF light can be further easily performed.
The following materials are used as the material having a high refractive index.
Al<sub>2</sub>O<sub>3</sub>: n=1.67
SiN<sub>x</sub>: n=2.03
TiO<sub>2</sub>: n=2.28
DLC: n=2.4
Ta<sub>2</sub>O<sub>5</sub>: n=2.14
ITO: n=2.00
<figref idref="DRAWINGS">FIGS. 8 and 9</figref> show the example of SiN<sub>x </sub>having the refractive index n=2.03. SiN<sub>x</sub>, is transparent over the range from the ultraviolet area to the infrared area and suitable for the semiconductor process, and also the stress control of the structure can be performed. Therefore, it is suitably used as the transmission type spatial light modulator <b>100</b>, so that it makes easy to manufacture a deflecting portion <b>39</b> having a prism angle θo of 25 to 30° and a rotational angle θr=±(5 to 15°).
When the prism angle θo is equal to 30°, the practical shape of the deflecting portion <b>39</b> may be designed so that light is totally reflected at the prism emission interface for the rotational angle θr=+0° or more, and light is transmitted at an emission angle θe=+40° and at the rotational angle θr=−5°. This shape will be described with respect to another embodiment described later.
<figref idref="DRAWINGS">FIG. 10</figref> is a plan view showing transmission type light modulators <b>100</b> of four pixels which are manufactured on a semiconductor substrate, <figref idref="DRAWINGS">FIG. 11</figref> is a cross-sectional view taken along XI-XI line of <figref idref="DRAWINGS">FIG. 10</figref> and <figref idref="DRAWINGS">FIG. 12</figref> is a cross-sectional view taken along XII-XII line of <figref idref="DRAWINGS">FIG. 10</figref>.
A first insulating layer <b>151</b> of SiO<sub>2 </sub>or the like is formed on a transparent substrate <b>150</b> of glass, quartz or the like, a driving circuit <b>152</b> based on a CMOS circuit is formed on the first insulating layer <b>151</b> by an Si semiconductor process, and a second insulating layer <b>153</b> of SiO<sub>2 </sub>or the like is formed on the driving circuit <b>152</b>. The driving circuit <b>152</b> is provided so that it is avoided from being provided just below the deflecting portion <b>39</b> comprising the transparent structure.
Metal film of aluminum or the like is laminated on the second insulating layer <b>153</b>, and the metal film is subjected to patterning, so that the lower electrodes <b>53</b>, <b>54</b> are provided every pixel. Furthermore, stopper film <b>58</b> is also formed from the metal film, and the end portion of the movable film <b>37</b> abuts against the stopper film <b>58</b> when the movable film <b>37</b> is inclined. The lower electrodes <b>53</b>, <b>54</b> are connected to the driving circuit <b>152</b> through contact holes <b>53</b><i>a</i>, <b>54</b><i>a </i>provided in the second insulating layer <b>153</b>, respectively.
Electrically conductive film is formed above the lower electrodes <b>53</b>, <b>54</b> through a gap <b>51</b>, and the electrically conductive film thus formed is subjected to patterning so that the movable film <b>37</b> of each pixel, hinges <b>32</b> linked to the movable film <b>37</b> and support portions <b>155</b> for supporting the movable film <b>37</b> through the hinges <b>32</b> on the transparent substrate <b>150</b>. A method of forming the electrically conductive film will be described later. A through hole <b>56</b> is formed at the center portion of the movable film <b>37</b> of each pixel, and the deflecting portion <b>39</b> formed of the transparent structure is formed above the through hole <b>56</b>.
The above structure is formed so that one deflecting portion <b>39</b> is provided every pixel, and these pixels are arranged one-dimensionally or two-dimensionally on the substrate, thereby constituting an spatial light modulation array. It is practically preferable that a one-pixel area is equal to 10 μm to 100 μm in square, and the opening portion (through hole <b>56</b>) is equal to 4 μm to 80 μm in square, however, they are not limited to these sizes.
<figref idref="DRAWINGS">FIGS. 13A and 13B</figref> are diagrams showing the operation of the transmission type light modulator <b>100</b>. When a potential difference is applied to the lower electrodes <b>53</b>, <b>54</b> with respect to the movable film <b>37</b>, electrostatic force occurs in the movable film <b>37</b>, and a rotational torque works around the hinge <b>32</b>. Accordingly, by controlling the potentials V<b>1</b>, V<b>2</b> of the respective electrodes <b>53</b>, <b>54</b>, the movable film <b>37</b> can be obliquely displaced to the right and left sides. At this time, the deflecting portion <b>39</b> is formed integrally with the movable film <b>37</b>, and thus the deflecting portion <b>39</b> is obliquely displaced in conformity with the oblique displacement of the movable film <b>37</b>. The inclination angles of the movable film <b>37</b> and the deflecting portion <b>39</b> are determined by the electrostatic force acting on each movable film <b>37</b> and the elastic force of the hinge <b>32</b>.
The output of the driving circuit <b>152</b> which can be independently controlled every pixel is connected to the lower electrodes <b>53</b>, <b>54</b> provided every pixel, and the potentials V<b>1</b>, V<b>2</b> are applied to the lower electrodes <b>53</b>, <b>54</b>. The movable film <b>37</b> is electrically connected to the stopper film <b>58</b> on the substrate <b>150</b> through the hinge <b>32</b> and the support portion <b>155</b>, and a potential Vm is applied to the movable film <b>37</b>. The supply of the potentials V<b>1</b>, V<b>2</b> is controlled by the driving circuit <b>152</b>, and for example 0V or 5V digital potential is supplied according to an image signal. In order to obliquely control the movable film <b>37</b> at a higher speed, it is preferable to carry out low-voltage digital driving of 0V or 3V.
The potential Vm may be controlled to be supplied from the driving circuit <b>152</b> provided every pixel or every plural pixels, or it may be controlled to be supplied from a common driving circuit of the whole array device. Furthermore, it may be controlled to be supplied from a circuit at the outside of the array device. The potential Vm is preferably controlled by analog potential. Here, when the absolute value of the potential difference between the movable film <b>37</b> and the electrode <b>53</b>, <b>54</b> is represented by V(<b>1</b>), V(<b>2</b>), the relationship with the control potential is represented as follows: <br />V(<b>1</b>)=|Vm-V<b>1</b>|<br />V(<b>2</b>)=|Vm-V<b>2</b>|
For V(<b>1</b>)=V(<b>2</b>)=0, external force occurring in the movable film <b>37</b> is equal to zero, and the state when the device has been formed is kept. That is, the movable film <b>37</b> and the deflecting portion <b>39</b> are substantially horizontal to the substrate <b>150</b>. This state is stabilized by the elastic force of the hinge <b>32</b>.
For V(<b>1</b>)=V(<b>2</b>)≠0, the electrostatic force occurring in the movable film <b>37</b> is also symmetrical with respect to the hinge <b>32</b>; Therefore, the state at the formation time of the device is kept, and the movable film <b>37</b> and the deflecting portion <b>39</b> are substantially horizontal to the substrate <b>150</b>.
When at least one of V(<b>1</b>) and V(<b>2</b>) is not equal to zero and also they are different from each other, the electrostatic force occurring in the movable film <b>37</b> is asymmetrical with respect to the hinge <b>32</b>. Accordingly, the movable film <b>37</b> and the deflecting portion <b>39</b> are obliquely displaced with respect to the substrate <b>150</b>. For example, in the case of V(<b>1</b>)>V(<b>2</b>), the electrostatic force acting between the electrode <b>53</b> and the left side of the movable film <b>37</b> is larger than the electrostatic force acting between the electrode <b>54</b> and the right side of the movable film <b>37</b> as shown in <figref idref="DRAWINGS">FIG. 13(</figref><i>a</i>), and the movable film <b>37</b> is inclined to the left side. That is, it is rotated in the counterclockwise direction. Conversely, in the case of V(<b>1</b>)<V(<b>2</b>), the electrostatic force acting between the electrode <b>54</b> and the right side of the movable film <b>37</b> is larger than the electrostatic force acting between the electrode <b>53</b> and the left side of the movable film <b>37</b> as shown in <figref idref="DRAWINGS">FIG. 13(</figref><i>b</i>), and thus the movable film <b>37</b> is inclined to the right side. That is, it is rotated in the clockwise direction. Accordingly, by properly controlling V(<b>1</b>) and V(<b>2</b>), the inclination angle θr of the movable film <b>37</b>, that is, the deflecting portion <b>39</b> can be freely controlled.
When V(<b>1</b>) or V(<b>2</b>) is sufficiently high and the electrostatic force contributing to the oblique displacement is larger than the elastic force of the hinge <b>32</b> or the electrostatic force occurring in the opposite direction, the movable film <b>37</b> and the deflecting portion <b>39</b> are obliquely displaced so that the end portion of the movable film <b>37</b> comes into contact with the stopper film <b>58</b>. Accordingly, the inclination angle at this time is geometrically determined by the length of the movable film <b>37</b> from the center portion of the hinge and the gap distance till the substrate. By properly selecting these shapes, a desired inclination angle can be freely designed. Here, even when the end portion of the movable film <b>37</b> comes into contact with the stopper film <b>58</b>, no short-circuit current flows because they are set to the same potential.
The present invention is not limited to the device construction, the electrode construction and the driving method of the above embodiment, and any construction may be adopted insofar as it is conformed with the subject matter of the present invention. For example, the device may be designed so that the inclination is carried out not by the vibration of the hinge, but by slack of a rib on which the end portion is supported. Furthermore, a driving electrode may be provided above the movable film <b>37</b> to intensify the electrostatic force (an embodiment having this construction will be described later). Furthermore, the movable film <b>37</b> may be driven in non-contact with the substrate <b>150</b> without providing any stopper film <b>58</b>.
<figref idref="DRAWINGS">FIGS. 14A to 14H</figref> and <figref idref="DRAWINGS">FIGS. 15A to 15H</figref> are diagrams showing the manufacturing process of the transmission type spatial light modulator shown in <figref idref="DRAWINGS">FIGS. 10 to 12</figref>. <figref idref="DRAWINGS">FIGS. 14A to 14H</figref> show the manufacturing process in the same cross-sectional view as <figref idref="DRAWINGS">FIG. 11</figref>, and <figref idref="DRAWINGS">FIGS. 15A to 15H</figref> show the manufacturing process in the same cross-sectional view as <figref idref="DRAWINGS">FIG. 12</figref>. <figref idref="DRAWINGS">FIGS. 14A and 15A</figref> are cross-sectional views showing the same manufacturing process. The same is applied to B to H.
First, as shown in <figref idref="DRAWINGS">FIG. 14A</figref> and <figref idref="DRAWINGS">FIG. 15A</figref>, the first insulating layer <b>151</b>, the driving circuit <b>152</b> formed of CMOS and the second insulating layer <b>153</b> are formed and laminated, the electrically conductive film is formed on the second insulating layer <b>153</b> and the stopper film <b>58</b> and the electrodes <b>53</b>, <b>54</b> are patterned from the electrically conductive film.
In order to form the driving circuit <b>152</b> of CMOS on the transparent substrate <b>150</b>, the following method is used. First, the driving circuit <b>152</b> of CMOS is formed on an SOI (Si on Insulator) substrate by an Si semiconductor process, and then the Si substrate is exfoliated from the insulating layer <b>15</b> below the driving circuit <b>152</b>. The driving circuit <b>152</b> and the insulating later <b>151</b> thus exfoliated are substituted onto a transparent substrate <b>150</b> by a transfer method or the like. Alternatively, the first insulating layer <b>151</b> is formed on the transparent substrate <b>150</b>, and then TFT (Thin Film Transistor) is directly formed to form the driving circuit <b>152</b>.
SiO<sub>2 </sub>is formed on the driving circuit <b>152</b> thus formed by PECVD to form the second insulating layer <b>153</b>. The contact holes <b>53</b><i>a</i>, <b>54</b><i>a </i>for connecting the output of the driving circuit <b>152</b> to each of the electrodes <b>53</b>, <b>54</b> are formed by a patterning treatment using photolithography and fluorine-based RIE etching. TiN thin film is formed as base film by sputtering (not shown), and subsequently tungsten (W) is formed by sputtering, whereby tungsten is embedded in the contact holes <b>53</b><i>a</i>, <b>54</b><i>a. </i>
Furthermore, the surface thereof is flattened to form the flat second insulating layer <b>153</b> having the contact holes <b>53</b><i>a</i>, <b>54</b><i>a </i>embedded with tungsten. Al serving as the electrically conductive film (preferably Al alloy containing metal having high melting point) is formed on the second insulating layer <b>153</b> by sputtering, and patterned into a desired electrode shape by photolithography and chlorine-based RIE etching, thereby forming the driving electrodes <b>53</b>, <b>54</b> and the stopper film <b>58</b>. At this time, the driving electrodes <b>53</b>, <b>54</b> are connected to the output of the driving circuit <b>152</b> through the contact holes <b>53</b><i>a</i>, <b>54</b><i>a. </i>
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14B</figref> and <figref idref="DRAWINGS">FIG. 15B</figref>, positive type resist film <b>156</b> is coated on the surface, and a portion thereof which will serve as the support portion <b>155</b> of the hinge <b>32</b> is patterned by photolithography and then subjected to hard-baking. The hard-baking is carried out at a temperature higher than 200° C. while DeepUV is irradiated. Accordingly, the shape thereof is kept even in the subsequent high-temperature process, and it is insoluble by resist exfoliating solvent. By coating and forming resist film, the resist surface is flattened irrespective of any step of the base film. The resist layer functions as a sacrifice layer, and is removed in the subsequent process. Accordingly, the film thickness of the resist after the hard-baking determines the gap <b>51</b> (see <figref idref="DRAWINGS">FIG. 2A</figref>) between the future lower electrodes <b>53</b>, <b>54</b> and the hinge <b>32</b> (and the movable film <b>37</b>).
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14C</figref> and <figref idref="DRAWINGS">FIG. 15C</figref>, electrically conductive film <b>157</b> of Al (preferably, Al alloy containing metal having a high melting point) is formed by sputtering, and only an opening portion (through hole <b>56</b> of <figref idref="DRAWINGS">FIG. 1</figref> and <figref idref="DRAWINGS">FIG. 10</figref>) is patterned into a desired shape by photolithography and chlorine-based RIE etching.
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14D</figref> and <figref idref="DRAWINGS">FIG. 15D</figref>, a transparent insulator formed of siO<sub>2 </sub>which will serve as the deflecting portion <b>39</b> is formed by PECVD, and subjected to a patterning so as to cover the periphery of the opening portion <b>56</b> by photolithography and fluorine-based RIE etching.
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14E</figref> and <figref idref="DRAWINGS">FIG. 15E</figref>, positive type resist film <b>159</b> is coated, and a resist structure <b>159</b> having the same shape as the deflecting portion <b>39</b> having a desired shape (a right triangular prism shape in the example of the figures) is formed on the transparent insulator <b>158</b> on the opening portion <b>56</b> by photolithography based on a gray-scale photomask.
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14F</figref> and <figref idref="DRAWINGS">FIG. 15F</figref>, the transparent insulator <b>158</b> is formed to have the same shape as the deflecting portion <b>39</b> by fluorine-based RIE etching. That is, the shape of the resist structure <b>159</b> is transferred to the transparent insulator <b>158</b> to thereby forming the deflecting portion <b>39</b>.
Subsequently, as shown in <figref idref="DRAWINGS">FIG. 14G</figref> and <figref idref="DRAWINGS">FIG. 15G</figref>, the electrically conductive film <b>157</b> is patterned by photolithography and chlorine-based RIE etching to form the hinge <b>32</b>, the support portion <b>155</b> and the movable film <b>37</b> from the electrically conductive film <b>157</b>.
Finally, as shown in <figref idref="DRAWINGS">FIG. 14H</figref> and <figref idref="DRAWINGS">FIG. 15H</figref>, the resist layer <b>156</b> serving as the sacrifice layer is removed by oxygen-based plasma etching (ashing) to form the gap <b>51</b>, thereby forming an spatial light modulator having a desired structure.
<figref idref="DRAWINGS">FIG. 16</figref> is a diagram showing a transmission type spatial light modulator <b>180</b> according to a second embodiment of the present invention. The transmission type spatial light modulator <b>180</b> of the second embodiment is different from the transmission type spatial light modulator <b>100</b> on in the construction of the driving member. <figref idref="DRAWINGS">FIG. 17</figref> shows a left-side inclination state (counterclockwise rotation state) of the transmission type spatial light modulator, and <figref idref="DRAWINGS">FIG. 18</figref> shows a right-side inclination state (clockwise rotation state) of the transmission type spatial light modulator <b>180</b>.
In the first embodiment, only the lower electrodes <b>53</b>, <b>54</b> are provided as the driving member <b>35</b>. However, in this embodiment, in addition to the lower electrodes <b>53</b>, <b>54</b>, upper electrodes <b>61</b> and <b>62</b> are disposed at both the sides of the hinge <b>32</b> (not shown) so as to sandwich the movable film <b>37</b> therebetween. In the example shown in <figref idref="DRAWINGS">FIG. 16</figref>, electrically conductive film <b>59</b> is formed on the whole lower surface of the movable film <b>37</b> because the movable film <b>37</b> is formed of insulating film, however, the movable film <b>37</b> itself may be formed of electrically conductive film as in the case of the first embodiment.
That is, in the transmission type spatial light modulator <b>180</b> of this embodiment, two lower electrodes <b>53</b>, <b>54</b> are arranged around a hinge at the lower side of the movable film <b>37</b> constituting a minute transparent optical member <b>33</b>, and also two upper electrodes <b>61</b>, <b>62</b> are arranged around a hinge at the upper side of the movable film <b>37</b>. That is, the torsion center of the hinge is located at the cross point between a pair of diagonal lines connecting diagonal electrodes (the lower electrodes <b>53</b>, <b>54</b>, the upper electrodes <b>61</b>, <b>62</b>) arranged at the four sides of upper and lower and right and left sides. Accordingly, the electrostatic force is effectively applied to the movable film <b>37</b> around the torsion center axis. The minute transparent optical member <b>33</b> can be actively driven to be clockwise rotated and counterclockwise rotated by the electrostatic force based on the electrodes arranged at the upper and lower sides.
As the basic operation, the transmission type spatial light modulator <b>180</b> swings and displaces the minute transparent optical member <b>33</b> by applying voltages to the lower electrodes <b>53</b>, <b>54</b>, the upper electrodes <b>61</b>, <b>62</b> and the electrically conductive film <b>59</b>.
In the transmission type spatial light modulator <b>180</b>, when a potential difference is applied to the first lower electrode <b>5</b>, the second lower electrode <b>54</b>, the first upper electrode <b>61</b> and the second upper electrode <b>62</b> with respect to the electrically conductive film <b>59</b>, electrostatic force occurs between each electrode and the electrically conductive film <b>59</b>, and a rotational torque works around the torsion center axis of the hinge. Accordingly, by controlling the potentials of the respective electrodes, the deflecting portion <b>39</b> can be rotationally displaced clockwise or counterclockwise.
For example, as shown in <figref idref="DRAWINGS">FIG. 16</figref>, the potential V<b>1</b> is applied to the first lower electrode <b>53</b>, the second upper electrode <b>62</b>, and the potential V<b>2</b> is applied to the second lower electrode <b>54</b> and the first upper electrode <b>61</b>, and the potential Vm is applied to the electrically conductive film <b>59</b>.
Here, the potential difference of V<b>1</b> from Vm is represented by V(<b>1</b>) and the potential difference of V<b>2</b> from Vm is represented by V(<b>2</b>). For V(<b>1</b>)=V(<b>2</b>)=0, the external force occurring in the minute transparent optical member <b>33</b> is equal to zero, the state at the time when the device is formed is kept, and the minute transparent optical member <b>33</b> is substantially horizontal to the substrate <b>31</b> as shown in <figref idref="DRAWINGS">FIG. 8</figref>. This state is stabilized by the elastic force of the hinge.
For V(<b>1</b>)=V(<b>2</b>)≠0, the electrostatic force occurring in the minute transparent optical member <b>33</b> is symmetrical with respect to the torsion center of the hinge, the state at the time when the device is formed is also kept, and the minute transparent optical member <b>33</b> is substantially horizontal to the substrate <b>31</b>.
When at least one of V(<b>1</b>) and V(<b>2</b>) is equal to zero and they are different from each other, the electrostatic force occurring in the minute transparent optical member <b>33</b> is asymmetrical with respect to the torsion center axis of the hinge, and the minute transparent optical member <b>33</b> is inclined with respect to the substrate <b>31</b>.
For example, for V(<b>1</b>)>V(<b>2</b>), the electrostatic force F generated by the first lower electrode <b>53</b> and the second upper electrode <b>62</b> is larger than the electrostatic force f generated by the second lower electrode <b>54</b> and the first upper electrode <b>61</b>, and the minute transparent optical member <b>33</b> is inclined to the left side as shown in <figref idref="DRAWINGS">FIG. 17</figref>. Conversely for V(<b>1</b>)-<V(<b>2</b>), the electrostatic force F generated by the second lower electrode <b>54</b> and the first upper electrode <b>61</b> is larger than the electrostatic force f generated by the first lower electrode <b>53</b> and the second upper electrode <b>62</b>, and the minute transparent optical member <b>33</b> is inclined to the right side.
At this time, in a case where V(<b>1</b>) and V(<b>2</b>) are sufficiently large, the minute transparent optical member <b>33</b> can be easily rotationally displaced in any direction from the flat state even when the difference between V(<b>1</b>) and V(<b>2</b>) is small. This means that when the potential to be controlled is set to V<b>1</b> and V<b>2</b>, the potential difference therebetween may be small. Therefore, the voltage of the control circuit can be reduced, and there is an advantage in cost performance and integration performance.
By properly supplying the potentials to V<b>1</b>, V<b>2</b>, Vm, the minute transparent optical member <b>33</b> can be displaced to any position, for example, in a clockwise direction, in a counterclockwise direction and in a flat direction by the electrostatic force occurring in each electrode and the elastic force of the hinge. Furthermore, the driving method at this time may be based on analog control (control for any displacement) or digital control (control for binary displacement).
With respect to the rotational driving operation described above, a proper rotation stopper (for example, the stopper film <b>58</b> of the first embodiment) is provided, and the minute transparent optical member <b>33</b> is rotationally displaced until it comes into contact with the stopper, whereby the rotational angle can be controlled with high precision. Furthermore, by using the linear area of the voltage-displacement characteristic, the minute transparent optical member <b>33</b> can be rotationally displaced so that the minute transparent optical member <b>33</b> does not come into contact with the stopper. In this case, there is no contact portion, and thus there occurs no problem such as attachment or the like, and the reliability can be enhanced. The electrode wiring and the displacing operation method of the minute transparent optical member <b>33</b> based on each potential control are embodiments, and thus the present invention is not limited to these embodiments.
In the transmission type spatial light modulator <b>180</b>, the driving member <b>35</b> obliquely displaces the minute transparent optical member <b>33</b> with the electrostatic force as described above, and thus the high-speed driving, the low-voltage driving and the low power-consumption driving can be performed.
Accordingly, according to the transmission type spatial light modulator <b>180</b>, the minute transparent optical member <b>33</b> for emitting light in a direction different from the incident light L<b>1</b> is supported by the support member so that it can be inclined, and the minute transparent optical member <b>33</b> is obliquely displaced by the electrical mechanical operation of the driving member <b>35</b> to thereby vary the light emission direction, so that the direction of the transmitted light and the light amount thereof can be controlled by a small displacement amount, and the high-speed deflection and the low-voltage driving can be implemented. Furthermore, in the case of the reflection type modulator, the light incident path and the light reflection path with respect to the device exist at the same surface side, and thus an optical system is required to avoid the interference between both the paths. However, according to the transmission type spatial light modulator <b>180</b> of this embodiment, the emission light is directed to the travel direction of the incident light and thus an optical system which is required in the case of the reflection type modulator is not required, and the construction of the peripheral optical system is simplified, so that the modulator can be miniaturized. Furthermore, as compared with the reflection type modulator, the effective light (ON light) and the unnecessary light (OFF light) can be more easily separated from each other, so that the stray light and the unnecessary light can be suppressed, and the contrast can be enhanced. Furthermore, there can be eliminated the wavelength-dependence which is observed in the interference type spatial light modulator using the Fabry-Perot effect or the like.
<figref idref="DRAWINGS">FIGS. 19A and 19B</figref> are cross-sectional views showing a modification <b>1</b> of the transmission type spatial light modulator according to the second embodiment in which a flexible flat plate is bent to displace a minute transparent optical member, and <figref idref="DRAWINGS">FIG. 20</figref> is a perspective view showing a modification <b>2</b> of the transmission type spatial light modulator which is equipped with a comb-drive.
The transmission type spatial light modulator <b>181</b> can adopts a structure shown in <figref idref="DRAWINGS">FIG. 19A</figref> to drive the minute transparent optical member <b>33</b>, for example. This driving structure has a minute transparent optical member <b>33</b> (comprising the movable film <b>37</b> and the deflecting portion <b>39</b>) for deflecting the incident light L<b>1</b>, at least one flexible flat plate <b>71</b> which is pivotably connected to the minute transparent optical member <b>33</b> at one end thereof and freely movably connected to the support portion <b>67</b> at the other end thereof, fixed electrodes <b>53</b>, <b>54</b>, <b>61</b>, <b>62</b> for displacing the minute transparent optical member <b>33</b>, and a movable electrode <b>75</b> provided on the flexible flat plate <b>71</b>. The fixed electrodes <b>53</b>, <b>54</b>, <b>61</b>, <b>62</b> are disposed so as to confront the upper and lower portions of the flexible flat plate <b>71</b> through gaps, and fixed to the substrate <b>31</b>. The flexible flat plate <b>71</b> is driven by the electrostatic force acting between the fixed electrodes <b>53</b>, <b>54</b>, <b>61</b>, <b>62</b> and the movable electrode <b>75</b>, thereby obliquely displacing the minute transparent optical member <b>33</b>.
In this transmission type spatial light modulator <b>181</b>, when a voltage is applied between the fixed electrode <b>53</b>, <b>54</b>, <b>61</b>, <b>62</b> and the movable electrode <b>75</b> which connects the minute transparent optical member <b>33</b> and the support portion <b>67</b> and is provided on the minute transparent optical member <b>33</b>, electrostatic force is generated between the fixed electrode <b>53</b>, <b>54</b>, <b>61</b>, <b>62</b> and the movable electrode <b>75</b>. The minute transparent optical member <b>33</b> is attracted to the substrate <b>31</b> (in an upward direction or downward direction), and as a result, the minute transparent optical member <b>33</b> is obliquely displaced as shown in <figref idref="DRAWINGS">FIG. 19B</figref>. In order to return the minute transparent optical member <b>33</b> to the state of <figref idref="DRAWINGS">FIG. 19A</figref>, the voltage between the movable electrode <b>75</b> and the fixed electrode <b>53</b>, . . . is set to zero.
Furthermore, the transmission type spatial light modulator may adopt a structure as shown in <figref idref="DRAWINGS">FIG. 20</figref> to drive the minute transparent optical member <b>33</b>. In the driving structure of the transmission type spatial light modulator <b>182</b>, the minute transparent optical member <b>33</b> is fixed at the center portion of the support member (hinge) <b>77</b>, and support shafts <b>79</b>, <b>79</b> are fixed to both the ends of a swing shaft <b>77</b> so as to be perpendicular to the swing shaft <b>77</b>. A so-called comb-drive <b>81</b> serving as the driving member is provided to each of the end portions of the support shafts <b>79</b>, <b>79</b>. In the comb-drive <b>81</b>, a comb-shaped upper electrode plate <b>81</b><i>a </i>and a comb-shaped lower electrode <b>81</b><i>b </i>are oriented so that the teeth thereof are mutually engaged with one another, and both the ends of the support shafts <b>79</b>, <b>79</b> are vertically moved by the electrostatic force acting between these confronting electrodes, so that the swing shaft <b>77</b> is rotated and the minute transparent optical member <b>33</b> can be freely rotated in both the clockwise and counterclockwise directions.
Next, a third embodiment of the transmission type spatial light modulator according to the present invention will be described. <figref idref="DRAWINGS">FIGS. 21A to 21C</figref> are cross-sectional views showing the third embodiment having a light shielding member, and <figref idref="DRAWINGS">FIGS. 22A and 22B</figref> are cross-sectional views showing a modification of the third embodiment in which the position of the light shielding member is different. In the following embodiments and modifications, the same members as shown in <figref idref="DRAWINGS">FIGS. 1 to 20</figref> are represented by the same reference numerals, and the duplicative description thereof is omitted.
A transmission type spatial light modulator <b>200</b> of this embodiment has light shielding member <b>83</b> in front of the light emission face of the minute transparent optical member <b>33</b>. The light shielding member <b>83</b> may be light shielding film formed on the front-surface protection substrate <b>57</b>, for example. The light shielding member <b>83</b> shields some emission light in a direction-variable range of light emitted from the minute transparent optical member <b>33</b>. The light shielding is carried out-by absorption or reflection.
In the transmission type spatial light modulator <b>200</b>, for example when the prism angle θo of the deflecting portion <b>39</b> having a refractive index n=1.5 is formed as shown in <figref idref="DRAWINGS">FIG. 21B</figref>, the inclination angle θr is equal to 0° and the emission angle θe of the deflected light is slightly less than 20° under an initial state where the driving member <b>35</b> is not actuated. At this time, the emission light L<b>2</b> is shielded by the light shielding member <b>83</b>. Furthermore, the emission angle θe of the deflected light is equal to 15° even when the driving member <b>35</b> is actuated and the inclination angle θr is equal to 15° as shown in <figref idref="DRAWINGS">FIG. 21A</figref>, and thus the emission light L<b>2</b> is shielded by the light shielding member <b>35</b>. On the other hand, when the driving member <b>35</b> is actuated and the inclination angle θr is equal to −15° as shown in <figref idref="DRAWINGS">FIG. 21C</figref>, the emission angle θe of the deflected light is greatly varied to 30°, so that the emission light L<b>2</b> is out of the light shielding member <b>83</b> and thus emitted from the front-surface protection substrate <b>57</b>.
Furthermore, as shown in <figref idref="DRAWINGS">FIGS. 22A and 22B</figref>, the light shielding member <b>83</b> may be provided at the opposite side to that in the case of <figref idref="DRAWINGS">FIGS. 21A to 21C</figref>. In this case, as shown in <figref idref="DRAWINGS">FIG. 22A</figref>, the emission light L<b>2</b> is shifted out of the light shielding member <b>83</b> and made to be emitted from the front-surface protection substrate <b>57</b> under the initial state where the driving member <b>35</b> is not actuated. Furthermore, as shown in <figref idref="DRAWINGS">FIG. 22B</figref>, when the driving member <b>35</b> is actuated and light emitted from the emission face of the minute transparent optical member <b>33</b> is greatly deflected, the emission light L<b>2</b> is shielded by the light shielding member <b>83</b>.
According to the transmission type spatial light modulator <b>200</b>, there is provided the light shielding member <b>83</b> for shielding some emission light emission light in the direction-variable range of the light emitted from the minute transparent optical member <b>33</b>. Accordingly, a desired area in the direction-variable range of light emitted from the minute transparent optical member <b>33</b> can be set as a light transmissible area or light shielding area. Furthermore, the driving member <b>35</b> obliquely displaces the minute transparent optical member <b>33</b> to displace the emission light with respect to the light shielding member <b>83</b>, thereby varying the light amount of transmission light. Therefore, the driving member is made to function as an optical switch which enables ON/OFF of light intensity or switching of a route in cooperation with the light deflecting operation based on the oblique displacement of the minute transparent optical member <b>33</b>.
Next, a fourth embodiment of the transmission type spatial light modulator according to the present invention will be described. <figref idref="DRAWINGS">FIGS. 23A and 23B</figref> are cross-sectional views showing the fourth embodiment in which the minute transparent optical member is obliquely driven to emit incident light from the emission face thereof or totally reflect the incident light from the emission face, and <figref idref="DRAWINGS">FIGS. 24A and 24B</figref> are cross-sectional views showing a modification of the fourth embodiment in which the shape of the minute transparent optical member is different.
The transmission type spatial light modulator <b>300</b> according to this embodiment is designed so that the emission face <b>89</b> of the deflecting portion <b>87</b> is swung in the vicinity of the critical angle with respect to the incident light L<b>1</b>. That is, the deflecting portion <b>87</b> of this embodiment is formed at the prism angle θo=45°. For example, in the case of glass having a refractive index n=1.5, the total reflection critical angle θcc is equal to about 42°, and the distance p from the prism corner portion to the apex angle portion is set to about 5 μm.
In the transmission type spatial light modulator <b>300</b>, an optical path correcting member <b>91</b> for making the incident angle and the emission angle substantially coincident with each other may be provided in front of the light emission face of the minute transparent optical member <b>85</b>. A prism is suitably used as the optical path correcting member <b>91</b>.
In the transmission spatial light modulator <b>300</b>, under the initial state where the driving member <b>35</b> is not actuated, the inclination angle θr=0°, and thus the incident light L<b>1</b> is incident to the emission face <b>89</b> at an angle of 45° larger than the critical angle of 42° as shown in <figref idref="DRAWINGS">FIG. 23A</figref>. Accordingly, the incident light L<b>1</b> is totally reflected from the emission face <b>89</b>, and thus no light is emitted from the emission face <b>89</b> to the optical path correcting member <b>91</b>. On the other hand, when the driving member <b>35</b> is actuated, as shown in <figref idref="DRAWINGS">FIG. 23B</figref>, the incident angle of the incident light L<b>1</b> to the emission face <b>89</b> is smaller than the critical angle, the emission light L<b>2</b> passes through the emission face <b>89</b> while being bent, further passes through the optical path correcting member <b>91</b> and then is emitted in parallel to the incident light L<b>1</b> (normally-off control).
According to the transmission type spatial light modulator <b>300</b>, the emission face <b>89</b> of the minute transparent optical member <b>85</b> is provided in the vicinity of the angle at which the incident light L<b>1</b> is totally reflected, and also not only the deflection of the incident light L<b>1</b>, but also the total reflection of the incident light L<b>1</b> can be performed. Accordingly, the deflected light is emitted from the opposite side to the light incident face of the minute transparent optical member <b>85</b>, and also the reflected light is emitted from the light incident face side of the minute transparent optical member <b>85</b>, so that the effective light (ON light) and the unnecessary light (OFF light) can be separated to the opposite sides with respect to the minute transparent optical member <b>85</b>.
Furthermore, the minute transparent optical member <b>85</b> is obliquely displaced by the driving member <b>35</b> to pass or totally reflect the incident light L<b>1</b>. Accordingly, the ON light and the OFF light can be separated to the opposite sides with respect to the minute transparent optical member <b>85</b> by obliquely displacing the minute transparent optical member <b>85</b> so that the incident angle of the incident light L<b>1</b> incident to the emission face <b>89</b> is smaller or larger than the critical angle. Since the light is totally reflected at the emission face <b>89</b> formed in the minute transparent optical member <b>85</b>, the total internal reflection (Total Internal Reflection) can be performed, so that light absorption can be reduced as compared with the reflection at the metal surface, and heating or degradation caused by high-intensity light can be prevented. Accordingly, an spatial light modulator adapted to light of a high-output light source can be implemented. Furthermore, the manufacturing process can be simplified as compared with the reflection based on formation of dielectric multi-layered film.
Furthermore, the optical path correcting member <b>91</b> for making the incident angle and the emission angle substantially coincident with each other is provided in front of the light emission face of the minute transparent optical member <b>85</b>. Therefore, the emission light L<b>2</b> (ON light) which is separated to the opposite side to the incident light L<b>1</b> with respect to the minute transparent optical member <b>85</b> can be made to straightly travel in the same direction as the incident light L<b>1</b>. Therefore, the optical design of the device using this modulator can be facilitated.
If a deflecting portion <b>93</b> having an asymmetric shape having a prism angle θo of about 35° is adopted as shown in <figref idref="DRAWINGS">FIGS. 24A and 24B</figref>, there could be perform the normally-off control under which the incident light L<b>1</b> is passed through the emission face <b>89</b> under the initial state as shown in <figref idref="DRAWINGS">FIG. 24A</figref>, and the incident light L<b>1</b> is totally reflected from the emission face <b>89</b> under the actuation state of the driving member <b>35</b> as shown in <figref idref="DRAWINGS">FIG. 24B</figref>.
Next, a fifth embodiment of the transmission type spatial light modulator according to the present invention will be described. <figref idref="DRAWINGS">FIG. 25</figref> is a cross-sectional view showing the fifth embodiment using a prism as the minute transparent optical member, <figref idref="DRAWINGS">FIG. 26</figref> is a cross-sectional view showing a modification <b>1</b> of the fifth embodiment in which optical path correcting member is provided, and <figref idref="DRAWINGS">FIG. 27</figref> is a cross-sectional view showing a modification <b>2</b> of the fifth embodiment in which a prism having a parallelogram shape is used.
In the transmission type spatial light modulator <b>400</b> of this embodiment, a deflecting portion <b>95</b> is designed in a prism-shape of a right-angled triangle having a total reflection face as shown in <figref idref="DRAWINGS">FIGS. 25A to 25D</figref>. In the deflecting portion <b>95</b>, one of the side portions between which the right angle is sandwiched is parallel to the movable film <b>37</b>. Accordingly, as shown in <figref idref="DRAWINGS">FIG. 25A</figref>, the incident light L<b>1</b> incident form the movable film <b>37</b> is totally reflected from the total reflection face <b>89</b> of the deflecting portion <b>95</b> at an angle of 90°, and emitted from the other side portion of the side portions between which the right angle is sandwiched. That is, the incident light L<b>1</b> is totally reflected by the prism, and deflected in a horizontal direction (in a direction parallel to the substrate <b>31</b>).
In this transmission type spatial light modulator <b>400</b>, as shown in <figref idref="DRAWINGS">FIG. 25B</figref>, when the refractive index n=1.5 and the oblique displacement of the movable film <b>37</b>, the inclination angle θr is equal to 10°, it is equal to 20° by the rotation in the positive and negative direction. In this case, the emission angle θe with respect to the inclination angle θe is also equal to 10°, and the deflection angle θs shown in <figref idref="DRAWINGS">FIG. 25C</figref> is equal to 20°. This means that a larger deflection angle (θs=20°) can be achieved at a smaller inclination angle (2θr=20°) as compared with the transmission type spatial light modulator <b>100</b> of the first embodiment which achieves the deflection angle θs=15° at the inclination angle 2θr=30°. Accordingly, a displacement H of 1.8 μm is achieved at the position located at a distance w=5.0 μm from the left end of the deflecting portion <b>95</b> as shown in <figref idref="DRAWINGS">FIG. 25D</figref>.
As an application of the transmission type spatial light modulator <b>400</b>, an optical path correcting member <b>91</b><i>a </i>and an optical path correcting member <b>91</b><i>b </i>may be provided at the light emission face side of the deflecting portion <b>95</b> so as to be spaced from each other through a gap as shown in <figref idref="DRAWINGS">FIG. 26</figref>. That is, an optical system is constructed by the combination of a movable prism and a fixed prism. According to such a construction, ON light can be emitted from the front-surface protection substrate <b>57</b> by the optical path correcting member <b>91</b><i>a </i>in the case of the inclination angle θr<0°, OFF light can be emitted in the horizontal direction in the case of the inclination angle θr=0°, and OFF light can be emitted from the substrate <b>31</b> by the optical path correcting member <b>91</b><i>b </i>in the case of the inclination angle θr>0°. That is, since the deflection angle θs can be increased by a small inclination angle θr, the deflected light is selectively introduced into the two optical path correcting member <b>91</b> which are spaced from each other, whereby the deflection in the same direction as the incident light L<b>1</b>, in the opposite direction to the incident light L<b>1</b> and in the vertical direction to the incident light L<b>1</b> can be surely performed.
Since the deflecting portion <b>95</b> has a prism shape, a large deflection angle (θs) can be achieved by a small inclination angle (θr). Furthermore, the reflection loss can be reduced, and the light absorption can be reduced as compared with the reflection at the metal surface. Still furthermore, since the deflection angle is increased, a margin can be easily taken (the design limit is moderated), and the degree of freedom of the optical design of an optical path or the like can be enhanced. Accordingly, for example, an optical communication device such as an optical switch for switching an optical path can be provided at a low price.
As a modification of the transmission type spatial light modulator <b>400</b>, two total reflection faces <b>89</b><i>a </i>and <b>89</b><i>b </i>are provided by using a parallelogram deflecting portion <b>97</b> as shown in <figref idref="DRAWINGS">FIG. 27</figref>. According to such a construction, ON light is emitted from the front-surface protection substrate <b>57</b> by the total reflection faces <b>89</b><i>a </i>and <b>89</b><i>b </i>in the case of the inclination angle θr<0°, OFF light can be emitted in an oblique upward direction from the total reflection face <b>89</b><i>b </i>by the total reflection face <b>89</b><i>a </i>in the case of the inclination angle θr=0°, and OFF light is emitted substantially in the horizontal direction from the total reflection face <b>89</b><i>b </i>by the total reflection face <b>89</b><i>a</i>. Accordingly, the OFF light is not returned to the incident side, and it can be escaped to an area which has less influence on the other areas, so that a stray light treatment can be excellently performed.
Next, a sixth embodiment of the transmission type spatial light modulator according to the present invention will be described. <figref idref="DRAWINGS">FIGS. 28A to 28C</figref> are cross-sectional views showing a sixth embodiment in which the light emission face of the minute transparent optical member has a curved-surface shape. In a transmission type spatial light modulator <b>500</b> of this embodiment, at least a part of the light incident face or light emission face of a minute transparent optical member <b>99</b> is designed in a curved-surface shape. In this embodiment, the light emission face is designed to have a convex curved-surface shape. That is, a deflecting portion <b>101</b> is designed in a convex-lens shape. The shape of the deflecting portion <b>101</b> may be designed in a concave-lens shape or it may be a Fresnel zone plate having a curved line portion which is coaxially different in curvature.
According to the transmission type spatial light modulator <b>500</b>, at least a part of the light incident face or light emission face is designed in a curved-surface shape. Therefore, the refractive index can be continuously varied, and also the refractive index difference in a refractive index variable range can be increased (as a result, the deflection angle difference can be increased).
Next, a seventh embodiment of the transmission type spatial light modulator according to the present invention will be described. <figref idref="DRAWINGS">FIGS. 29A to 29C</figref> are cross-sectional views showing a seventh embodiment in which the minute transparent optical member has a refractive index distribution, and <figref idref="DRAWINGS">FIGS. 30A to 30C</figref> are cross-sectional views showing a modification of the seventh embodiment in which a refraction interface is designed to be a curved surface.
In a transmission type spatial light modulator <b>600</b> of this embodiment, a minute transparent optical member <b>103</b> has a refractive index distribution which is different in refractive index in the travel direction of light. In addition, the light deflecting direction based on the refractive index distribution is not parallel to the light travel direction, and thus both the directions are different from each other. The minute transparent optical member <b>103</b> having such a characteristic can be constructed by designing the whole of the minute transparent optical member <b>103</b> or only the deflecting portion in a rectangular sectional shape as shown in <figref idref="DRAWINGS">FIGS. 29A to 29C</figref>, and making the refractive index n<b>1</b> of an upper medium <b>103</b><i>a </i>and the refractive index n<b>2</b> of a lower medium <b>103</b><i>b </i>different from each other (for example, n<b>1</b>>n<b>2</b>) with a pair of diagonal lines as the boundary therebetween.
In the transmission type spatial light modulator <b>600</b>, as shown in <figref idref="DRAWINGS">FIG. 29B</figref>, under the initial condition that the driving member <b>35</b> is not actuated, the emission angle of the deflected light is θe<b>1</b> for the inclination angle θr=0°. As shown in <figref idref="DRAWINGS">FIG. 29A</figref>, the driving member <b>35</b> is actuated, and the emission angle of the deflected light is θe<b>2</b> for the inclination angle θr<0°. Furthermore, as shown in <figref idref="DRAWINGS">FIG. 29C</figref>, the driving member <b>35</b> is actuated, and the emission angle of the deflected light is θe<b>3</b> for the inclination angle θr>0°. Here, by setting the refractive indexes n<b>1</b>, n<b>2</b> and the attachment face angle of the media <b>103</b><i>a</i>, <b>103</b><i>b</i>, “θe<b>1</b>≠θe<b>2</b><θe<b>3</b>” can be established. That is, any deflection range can be set by setting a refractive index distribution or the like.
According to a transmission type spatial light modulator <b>600</b>, a minute transparent optical member <b>103</b> has a refractive index distribution in which the refractive index is varied in the light travel direction, and also the light deflection direction achieved by the refractive index distribution is not parallel to the light travel direction, so that any deflection range can be set by using a flat-plate type minute transparent optical member <b>103</b>. Furthermore, the thickness of the minute transparent optical member <b>103</b> having a desired deflection range can be reduced, so that the modulator can be designed to be light in weight and have high-speed response.
As a modification of the transmission type spatial light modulator <b>600</b>, as shown in <figref idref="DRAWINGS">FIGS. 30A to 30C</figref>, a minute transparent optical member <b>105</b> is achieved by laminating two or more media (<b>105</b><i>a</i>, <b>105</b><i>b</i>, <b>105</b><i>c</i>, <b>105</b><i>d</i>). In this case, the respective media are laminated so that the interfaces thereof are arranged in a coaxial arcuate shape, and they are designed so that a medium located at a near position to the center has a higher refractive index. This construction has an effect of further increasing the angle difference between (θe<b>1</b>≠θe<b>2</b>) and (θe<b>3</b>) as compared with the construction shown in <figref idref="DRAWINGS">FIGS. 29A to 29C</figref>.
Next, an eighth embodiment of the transmission type spatial light modulation array device according to the present invention will be described. <figref idref="DRAWINGS">FIG. 31</figref> is a cross-sectional view showing the transmission type spatial light modulation array device according to the eighth embodiment in which micro-lenses are integrated, and <figref idref="DRAWINGS">FIG. 32</figref> is a cross-sectional view showing a modification of the transmission type spatial light modulation array device shown in <figref idref="DRAWINGS">FIG. 31</figref> which is equipped with two-stage micro-lenses.
The above transmission type spatial light modulators (<b>100</b>, <b>180</b>, <b>181</b>, <b>182</b>, <b>200</b>, <b>300</b>, <b>400</b>, <b>500</b> or <b>600</b>) may be arranged one-dimensionally or two-dimensionally to constitute a transmission type spatial light modulation array device <b>700</b>. For example, the transmission type spatial light modulators <b>300</b> having the same structure are arranged one-dimensionally or two-dimensionally on the same movable element substrate <b>111</b>, whereby the transmission type spatial light modulation array device <b>700</b> functions as one transmission type light deflecting device.
A transparent insulating film <b>113</b> is laminated on a movable element device <b>111</b>, and the above driving circuits (CMOS or the like) <b>115</b> are respectively formed in the other area than the light transmission area of the transparent insulating film <b>113</b> in connection with the respective transmission type spatial light modulators <b>300</b>. Furthermore, a micro-lens array <b>117</b> is disposed and joined to the light incident face of the movable element substrate <b>111</b> so as to confront the light incident face of the movable element substrate <b>111</b> in parallel. The micro-lens array <b>117</b> has plural micro-lenses <b>117</b><i>a </i>corresponding to the respective transmission type spatial light modulators <b>300</b>.
According to the transmission type spatial light modulation array device <b>700</b>, the transmission type spatial light modulators described above (<b>100</b>, <b>180</b>, <b>181</b>, <b>182</b>, <b>200</b>, <b>300</b>, <b>400</b>, <b>500</b> or <b>600</b>) are one-dimensionally or two-dimensionally arranged and thus they function as one light modulation device. Therefore, they can optically modulate high-density pixels at high speed in an application to a light exposure head, a display or the like. In addition, many transmission type spatial light modulators can be arranged with the same quality and high precision by the semiconductor manufacturing process, so that image display, etc. can be performed with high quality and high precision while aligning emission light.
The micro-lens array <b>117</b> having the plural micro-lenses <b>117</b><i>a </i>corresponding to the respective transmission type spatial light modulators are arranged at the light incident face so as to confront the light incident face, and thus the incident light flux can be narrowed down, so that the minute transparent optical member is miniaturized and reduced in weight, and the high-speed driving, the low-voltage driving and the low power-consumption driving can be performed. Furthermore, as compared with a case where no micro-lens <b>117</b><i>a </i>is used, the minute transparent optical member can be formed in a small area, and thus the driving circuit area can be more easily secured when compared on the assumption of the same substrate area.
As a modification of the transmission type spatial light modulation array device <b>700</b>, other micro-lenses <b>117</b><i>b </i>are formed on the same optical axis as the micro-lenses <b>117</b><i>a </i>as shown in <figref idref="DRAWINGS">FIG. 32</figref>. In this construction, the incident light flux is passed through the micro-lenses <b>117</b><i>a</i>, whereby the light converged to the focusing point is passed through the other micro-lenses <b>117</b><i>b </i>as divergent light and collimated light is made incident to the movable element substrate <b>111</b>.
Next, a ninth embodiment adopting the transmission type spatial light modulation array device of this invention as an exposure device will be described. <figref idref="DRAWINGS">FIG. 33</figref> is a diagram showing the construction of the exposure device of the ninth embodiment which uses the transmission type spatial light modulation array device, <figref idref="DRAWINGS">FIG. 34</figref> is a block diagram showing the exposure device shown in <figref idref="DRAWINGS">FIG. 33</figref> and <figref idref="DRAWINGS">FIG. 35</figref> is a diagram showing the optical path of the exposure device shown in <figref idref="DRAWINGS">FIG. 33</figref>.
The transmission type spatial light modulation array device described above is suitably applicable to the exposure device <b>800</b> shown in <figref idref="DRAWINGS">FIG. 33</figref>, for example. The transmission type spatial light modulation array device <b>900</b> may be constructed by providing the micro-lens array <b>117</b> to the transmission type spatial light modulators <b>100</b>. The exposure device <b>800</b> is equipped with a drum <b>123</b> for holding an exposure target <b>121</b> while adsorbing the exposure target <b>121</b> on the outer peripheral surface thereof, and an auxiliary scanning unit <b>127</b> which is freely movably supported by a guide shaft <b>125</b> extending along the rotational axis of the exposure device <b>3</b>. The drum <b>123</b> is counterclockwise rotated by a rotational driving motor (not shown). The auxiliary scanning unit <b>127</b> is moved in the right-and-left direction of <figref idref="DRAWINGS">FIG. 33</figref> by a horizontal driving motor (not shown). Here, with respect to the exposure target <b>121</b>, a D-direction based on the rotation of the drum <b>123</b> corresponds to a main scanning direction, and an L-direction based on the movement of the auxiliary scanning unit <b>127</b> corresponds to an auxiliary scanning direction.
As shown in <figref idref="DRAWINGS">FIG. 34</figref>, the auxiliary scanning unit <b>127</b> has a light-source/SLM (optical modulating) unit <b>129</b> and an imaging lens system <b>131</b>. The rotational position of the drum <b>123</b> is detected by a main scanning position detector <b>133</b>, and the moving position of the auxiliary scanning unit <b>127</b> is detected by an auxiliary scanning position detector <b>135</b>. The position signals detected by the main scanning position detector <b>133</b> and the auxiliary scanning position detector <b>135</b> are input to a signal generator <b>137</b>. The signal generator <b>137</b> outputs a modulation signal and a light source signal to the light-source/SLM unit <b>129</b> in accordance with an image signal transmitted from a superordinate controller on the basis of these position signals. The imaging lens system <b>131</b> is constructed by combined zoom lenses <b>131</b><i>a</i>, <b>1341</b><i>b </i>for imaging a laser beam modulated and emitted from the light-source/SLM unit <b>129</b> onto the surface of the exposure target <b>121</b> while varying the magnification thereof.
In the light-source/SLM unit <b>129</b>, plural transmission type spatial light modulators <b>100</b> are arranged in the auxiliary scanning direction in the transmission type spatial light modulation array device <b>900</b>. An optical path correcting member <b>141</b> is disposed at the light incident face side of the transmission type spatial light modulation array device <b>900</b>, and the optical path correcting member <b>141</b> totally reflects or transmits deflected light emitted from the transmission type modulation array device <b>900</b> by the emission face <b>141</b><i>a</i>, thereby separating the light into effective light (ON light) and unnecessary light (OFF light).
Accordingly, when the exposure target <b>121</b> and the auxiliary scanning unit <b>127</b> are relatively moved in the direction (main scanning direction) perpendicular to the arrangement direction of the transmission type spatial light modulators <b>100</b>, one-line pixels whose number is equal to the arrangement number of the transmission type spatial light modulators <b>100</b> can be exposed to ON light emitted form the emission face <b>141</b><i>a</i>in the same direction as described above. Image signals of one line are transmitted as modulation signals and light source signals to the transmission type spatial light modulators <b>100</b> together with the movement of the exposure target <b>121</b> in the main scanning direction, and the respective transmission type spatial light modulators <b>100</b> are controlled to be turned on and off. Accordingly, the exposure light emitted from the auxiliary scanning unit <b>127</b> is turned on and off, and exposure control is carried out on the exposure target <b>121</b> every pixels whose number is equal to the number of the transmission type spatial light modulators <b>100</b> in the main scanning direction, thereby carrying out the scan-exposure operation of one line. Thereafter, the auxiliary scanning unit <b>127</b> is moved in the auxiliary scanning direction, and the subsequent one line is successively exposed to light in the same manner.
As described above, according to the exposure device <b>800</b> having the transmission type spatial light modulation array device <b>900</b>, the incident light L<b>1</b> is deflected at high speed by the transmission type spatial light modulation array device <b>900</b>, and the deflected light is separated into ON light and OFF light by the optical path correcting member <b>141</b>, whereby exposure or image recording can be carried out on the exposure target <b>121</b>. Furthermore, the deflected light can be emitted substantially in the straight direction by using the transmission type spatial light modulators <b>100</b>, and it is not required to bend the optical path at a large angle, which is needed in the case of the reflection type spatial light modulator. Therefore, the optical system around the modulator can be disposed linearly and thus the compact design of the device can be facilitated.
The exposure target <b>121</b> may be not only a recording medium held bon the drum <b>123</b>, but also a screen. In this case, the driving of the transmission type spatial light modulation array device <b>900</b> is controlled in accordance with an image signal, and emission light is projected onto the screen through a projection lens. Accordingly, a projector using the transmission type spatial light modulators can be achieved.
According to the transmission type spatial light modulator and the transmission type spatial light modulation array device, the direction and light amount of the transmitted light can be controlled by a small displacement amount, and high-speed deflection and low-voltage driving can be performed. Therefore, they are applicable to high-precision and high-resolution exposure head, display, etc.
Contents4
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| Cleared by OIPE CSRL194 | L194 | |
| IFW Scan & PACR Auto Security ReviewSCAN | SCAN | |
| Information Disclosure Statement consideredIDSC | IDSC | |
| Information Disclosure Statement (IDS) FiledM844 | M844 | |
| Information Disclosure Statement (IDS) FiledWIDS | WIDS | |
| Initial Exam Team nnIEXX | IEXX |
9 legal events, as the office reported them to INPADOC
Over the term
Point at a mark for the eventEvents
| Event | Code | |
|---|---|---|
| Lapsed due to failure to pay maintenance feeLapsedFP | FP | |
| Information on status: patent discontinuationPATENT EXPIRED DUE TO NONPAYMENT OF MAINTENANCE FEES UNDER 37 CFR 1.362STCH | STCH | |
| Information on status: patent discontinuationPATENT EXPIRED DUE TO NONPAYMENT OF MAINTENANCE FEES UNDER 37 CFR 1.362STCH | STCH | |
| Lapse for failure to pay maintenance feesLapsedLAPS | LAPS | |
| Maintenance fee reminder mailedREMI | REMI | |
| Fee paymentFPAY | FPAY | |
| AssignmentAS | AS | |
| AssignmentAS | AS | |
| AssignmentAS | AS |
Numbers
- Publication
- 07359103
- Publication, DOCDB
- 7359103
- Publication, EPODOC
- US7359103
- Application
- 11145926
- Application, DOCDB
- 14592605
- Application, EPODOC
- US20050145926
Titles
- English
- Transmission type spatial light modulator and transmission type spatial light modulation array device
Patent term adjustment
- A delay
- +295 daysthe office missed an examination deadline
- Applicant delay
- −29 days
- Net adjustment
- 266 days
Classification
- CPC, 1
- G02B26/0891
- IPC, 4
- G02B26 00
- G02B26 08
- B81B3 00
- B81B7 04
- USPC, 4
- 359237000
- 359247000
- 359298000
- 359302000